Abstract

Magnetic and quadrupole moments of the $7/{2}^{+}$ ground state in $^{133}\mathrm{Sb}$ and the $({7}^{\ensuremath{-}})$ isomer in $^{134}\mathrm{Sb}$ have been measured by collinear laser spectroscopy to investigate the single-particle behavior above the doubly magic nucleus $^{132}\mathrm{Sn}$. The comparison of experimental data of the $7/{2}^{+}$ states in $^{133}\mathrm{Sb}$ and neighboring $N=82$ isotones to shell-model calculations reveals the sensitivity of magnetic moments to the splitting of the spin-orbit partners $\ensuremath{\pi}0{g}_{9/2}$ and $\ensuremath{\pi}0{g}_{7/2}$ across the proton shell closure at $Z=50$. In contrast, quadrupole moments of the $N=82$ isotones are insensitive to cross-shell excitations, but require the full proton model space from $Z=50\phantom{\rule{4.pt}{0ex}}\text{to}\phantom{\rule{4.pt}{0ex}}82$ for their accurate description. In fact, the linear trend of the quadrupole moment follows approximately the expectation of the seniority scheme when filling the $\ensuremath{\pi}0{g}_{7/2}$ orbital. As far as the isomer in $^{134}\mathrm{Sb}$ is concerned, its electromagnetic moments can be perfectly described by the additivity rule employing the moments of $^{133}\mathrm{Sb}$ and $^{133}\mathrm{Sn}$, respectively. These findings agree with shell-model calculations and thus confirm the weak coupling between the valence proton and neutron in $^{134}\mathrm{Sb}$.

Highlights

  • Out of the over 3000 atomic nuclei discovered so far [1], only about ten represent nuclides with closed nuclear shells for both protons and neutrons

  • The objective of this research was to measure the electromagnetic moments of 133,134Sb with high-resolution laser spectroscopy in order to establish a better understanding of nuclear structure above the doubly magic nucleus 132Sn

  • An increased occupancy of the 0g7/2 orbital reduces the probability of core excitations from 0g9/2 to 0g7/2 and limits the effect from core polarization. 141Pr does not seem to follow the general trend, but its experimental uncertainty is too large for firm conclusions

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Summary

Introduction

Out of the over 3000 atomic nuclei discovered so far [1], only about ten represent nuclides with closed nuclear shells for both protons and neutrons. Such rare exemplars, found at the traditional shell closures Z, N = 2, 8, 20, 28, 50, 82, or 126, are called doubly magic nuclei. Deviations from the Schmidt moment give insights on the purity of the nuclear configuration, while electric quadrupole moments allow the investigation of second order core-polarization effects. Examples for this can be found in 41,49Sc [4]

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